The impact of a 126 GeV Higgs on the neutralino mass

We highlight the differences of the dark matter sector between the constrained minimal supersymmetric SM (CMSSM) and the next-to-minimal supersymmetric SM (NMSSM) including the 126 GeV Higgs boson using GUT scale parameters. In the dark matter sector the two models are quite orthogonal: in the CMSSM...

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Main Authors: C. Beskidt, W. de Boer, D.I. Kazakov
Format: Article
Language:English
Published: Elsevier 2014-11-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269314005784
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spelling doaj-39c613164fee430bb59ec353238cfa7d2020-11-24T21:35:28ZengElsevierPhysics Letters B0370-26932014-11-01738505511The impact of a 126 GeV Higgs on the neutralino massC. Beskidt0W. de Boer1D.I. Kazakov2Institut für Experimentelle Kernphysik, Karlsruhe Institute of Technology, P.O. Box 6980, 76128 Karlsruhe, GermanyInstitut für Experimentelle Kernphysik, Karlsruhe Institute of Technology, P.O. Box 6980, 76128 Karlsruhe, Germany; Corresponding author.Institut für Experimentelle Kernphysik, Karlsruhe Institute of Technology, P.O. Box 6980, 76128 Karlsruhe, Germany; Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, 141980, 6 Joliot-Curie, Dubna, Moscow Region, RussiaWe highlight the differences of the dark matter sector between the constrained minimal supersymmetric SM (CMSSM) and the next-to-minimal supersymmetric SM (NMSSM) including the 126 GeV Higgs boson using GUT scale parameters. In the dark matter sector the two models are quite orthogonal: in the CMSSM the WIMP is largely a bino and requires large masses from the LHC constraints. In the NMSSM the WIMP has a large singlino component and is therefore independent of the LHC SUSY mass limits. The light NMSSM neutralino mass range is of interest for the hints concerning light WIMPs in the Fermi data. Such low mass WIMPs cannot be explained in the CMSSM. Furthermore, prospects for discovery of XENON1T and LHC at 14 TeV are given. Keywords: Supersymmetry, Dark matter, Higgs bosonhttp://www.sciencedirect.com/science/article/pii/S0370269314005784
collection DOAJ
language English
format Article
sources DOAJ
author C. Beskidt
W. de Boer
D.I. Kazakov
spellingShingle C. Beskidt
W. de Boer
D.I. Kazakov
The impact of a 126 GeV Higgs on the neutralino mass
Physics Letters B
author_facet C. Beskidt
W. de Boer
D.I. Kazakov
author_sort C. Beskidt
title The impact of a 126 GeV Higgs on the neutralino mass
title_short The impact of a 126 GeV Higgs on the neutralino mass
title_full The impact of a 126 GeV Higgs on the neutralino mass
title_fullStr The impact of a 126 GeV Higgs on the neutralino mass
title_full_unstemmed The impact of a 126 GeV Higgs on the neutralino mass
title_sort impact of a 126 gev higgs on the neutralino mass
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2014-11-01
description We highlight the differences of the dark matter sector between the constrained minimal supersymmetric SM (CMSSM) and the next-to-minimal supersymmetric SM (NMSSM) including the 126 GeV Higgs boson using GUT scale parameters. In the dark matter sector the two models are quite orthogonal: in the CMSSM the WIMP is largely a bino and requires large masses from the LHC constraints. In the NMSSM the WIMP has a large singlino component and is therefore independent of the LHC SUSY mass limits. The light NMSSM neutralino mass range is of interest for the hints concerning light WIMPs in the Fermi data. Such low mass WIMPs cannot be explained in the CMSSM. Furthermore, prospects for discovery of XENON1T and LHC at 14 TeV are given. Keywords: Supersymmetry, Dark matter, Higgs boson
url http://www.sciencedirect.com/science/article/pii/S0370269314005784
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